Hadronic D decays involving even-parity light mesons

被引:42
作者
Cheng, Hai-Yang [1 ,2 ]
Chiang, Cheng-Wei [1 ,3 ,4 ]
机构
[1] Acad Sinica, Inst Phys, Taipei 115, Taiwan
[2] Brookhaven Natl Lab, Dept Phys, Upton, NY 11973 USA
[3] Natl Cent Univ, Dept Phys, Chungli 320, Taiwan
[4] Natl Cent Univ, Ctr Math & Theoret Phys, Chungli 320, Taiwan
关键词
MULTIQUARK HADRONS; NONLEPTONIC DECAYS; CHARM MESONS; WEAK DECAYS; QUARK; PSEUDOSCALAR; SYMMETRY; D-S(+); HEAVY; FACTORIZATION;
D O I
10.1103/PhysRevD.81.074031
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We study the hadronic D meson decays into a pseudoscalar meson P and an even-parity meson M, where M represents a scalar meson S, an axial-vector meson A, or a tensor meson T. These decays are first analyzed in the flavor-diagram approach. Fits to the SP modes with S being a nonstrange scalar meson show that neither the simple q (q) over bar picture nor the q(2)(q) over bar (2) scheme is favored by data. Current measurements on the AP decays are insufficient for a meaningful analysis. Some TP data are inconsistent with the others. In certain cases, the W-annihilation diagrams indicated by the data are unexpectedly large. As a comparison, we also compute their decay rates in the factorization approach using form factors extracted from the covariant light-front model. We find that factorization works well for Cabibbo-allowed D+ -> SP, AP decays free of the weak annihilation contributions (W-exchange or W-annihilation). For the other SP and AP modes, it is necessary to include weak annihilation contributions to account for the data. However, factorization fails for D -> TP decays for some unknown reason; the predicted rates are in general too small by at least 2 orders of magnitude compared to experiment. We also examine the finite-width effects of resonances. Some decay modes which are kinematically forbidden become physically allowed due to the finite width of the resonance. We show that the branching fraction of D+ -> sigma pi(+) extracted from three-body decays is enhanced by a factor of 2, whereas B(D-0 -> f(2)(1270)(K) over bar (0)) is reduced by a factor of 4 by finite-width effects.
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页数:19
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